Abstract

An analysis of nuclear reactions in the intermediate energy range has been made in terms of the statistical theory of nuclear reactions using the Fermi gas level density, $\mathrm{const}\ifmmode\times\else\texttimes\fi{}\mathrm{exp}[{(\mathrm{aE})}^{\frac{1}{2}}]$, where $E$ is the energy of excitation. The quantity, $a$, determined from excitation function experiments and from the ($\ensuremath{\alpha}, p$) reaction at 40 Mev shows an anomalous behavior when plotted against atomic number, $A$. On the other hand, the values of $a$ determined from several inelastic scattering and reaction experiments show the correct dependence on $A$. The effects of noncompound-nucleus processes are discussed.

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